The Rietveld refinement of synchrotron and neutron diffraction patterns and the structure of LiCuSO4F is shown in Figure 1.
The competitive formation of disordered or ordered triplite phase was evaluated through DFT calculations (Figure 2c). We demonstrate that both ordered CuM1 and CuM2 triplite LiCuSO4F polymorphs are thermodynamically equivalent, and more stable than either “tavorite” or “disordered triplite” polymorphs. The enthalpy governs the formation of an ordered LiCuSO4F triplite. This contrasts with the entropy-driven formation of LiFeSO4F disordered triplite in which all Fe-Li distributions are energetically equivalent.
This new phase was tested for its electrochemical activity towards Li by assembling, in an argon dry box , LiCuSO4F/Li Swagelok-type cells using a 1M LiPF6 solution in 1:1:3 EC : PC : DMC electrolyte. The cells were charged to either 4.9 V or 5.2 V at different rates via a VMP system, but no sign of redox activity could be detected in the voltage composition curves. This means that no Li can be removed from this structure till 5.2V, the voltage at which we found the electrolyte copiously decomposes although DFT calculations shows the feasibility to stabilize an intermediate ordered Li0.5CuSO4F phase (Figure 2d). The electrochemical potentials computed for the two consecutive delithiation processes: LiCuSO4F – 0.5Li Li0.5CuSO4F and Li0.5CuSO4F – 0.5Li CuSO4F are 5.15 V and 5.40 V, respectively. This could not be confirmed experimentally owing to the lack of suitable electrolytes although we cannot eliminate kinetic issues associated to the poor Li ionic conductivity in LiCuSO4F (not shown here). Thus, the attractiveness of this new phase is limited application-wise.
Nevertheless bearing in mind the richness of sulfate-/phosphate-based polyanionic electrodes adopting either the tavorite or disordered triplite structures, we believe that such a finding will contribute further in the understanding of these technologically important compounds.
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